• Acta Physica Sinica
  • Vol. 68, Issue 18, 185201-1 (2019)
Zhong-Heng Liu, Guang-Wei Meng*, and Ying-Kui Zhao*
DOI: 10.7498/aps.68.20182211 Cite this Article
Zhong-Heng Liu, Guang-Wei Meng, Ying-Kui Zhao. Movement of ablated high-Z plasmas [J]. Acta Physica Sinica, 2019, 68(18): 185201-1 Copy Citation Text show less
(a) Simplification of physical model; (b) one-dimensional model; (c) the wave system.(a)物理模型的简化; (b)一维模型的示意图; (c)波系示意图
Fig. 1. (a) Simplification of physical model; (b) one-dimensional model; (c) the wave system.(a)物理模型的简化; (b)一维模型的示意图; (c)波系示意图
(a) Temperature and density versus distance; (b)versus ; (c) ablation pressure versus time; (d) ablated mass versus time.(a)辐射温度和Au等离子体密度的空间分布; (b)随辐射源温度的变化; (c)烧蚀压和(d)烧蚀质量随时间的变化
Fig. 1. (a) Temperature and density versus distance; (b) versus ; (c) ablation pressure versus time; (d) ablated mass versus time. (a)辐射温度和Au等离子体密度的空间分布; (b) 随辐射源温度 的变化; (c)烧蚀压和(d)烧蚀质量随时间的变化
(a) Displacement and (b) velocity of the left interface of Au plasmas versus time under the condition of different and . The reverse time and distance of Au plasmas versus (c) with and (d) with .Au等离子体的左界面在不同和条件下的(a)位移和(b)速度随时间的变化; 折返时间和折返距离分别随(c) (取), (d) (取)的变化
Fig. 2. (a) Displacement and (b) velocity of the left interface of Au plasmas versus time under the condition of different and . The reverse time and distance of Au plasmas versus (c) with and (d) with . Au等离子体的左界面在不同 和 条件下的(a)位移和(b)速度随时间的变化; 折返时间和折返距离分别随(c) (取 ), (d) (取 )的变化
Temperature, velocity, density and pressure versus cell number n at 0.02 μs under the condition of and .在, 条件下, 时网格的温度、速度、密度和压强随网格编号n的变化
Fig. 3. Temperature, velocity, density and pressure versus cell number n at 0.02 μs under the condition of and . 在 , 条件下, 时网格的温度、速度、密度和压强随网格编号n的变化
Theoretical prediction (with ) of (a) reverse time and (b) reverse distance versus .理论预测(取)的(a)折返时间和(b)折返距离随辐射源温度的变化
Fig. 4. Theoretical prediction (with ) of (a) reverse time and (b) reverse distance versus . 理论预测(取 )的(a)折返时间和(b)折返距离随辐射源温度 的变化
Reverse time and distance versus Tr under different density of (a) 0.05, (b) 0.5, and (c) 1 g·cm–3. (d) ξ and η versus .折返时间和折返距离分别在不同的密度(a) 0.05, (b) 0.5, (c) 1 g·cm–3下与辐射源温度Tr的变化关系; (d) 参数ξ和η随的变化
Fig. 5. Reverse time and distance versus Tr under different density of (a) 0.05, (b) 0.5, and (c) 1 g·cm–3. (d) ξ and η versus . 折返时间和折返距离分别在不同的密度 (a) 0.05, (b) 0.5, (c) 1 g·cm–3下与辐射源温度Tr的变化关系; (d) 参数ξη随 的变化
(a) The peak temperature and (b) of reverse time and distance versus .折返时间和折返距离的(a)峰值温度和(b)峰值温度的三次方随密度的变化
Fig. 6. (a) The peak temperature and (b) of reverse time and distance versus . 折返时间和折返距离的(a)峰值温度 和(b)峰值温度的三次方 随密度 的变化
Zhong-Heng Liu, Guang-Wei Meng, Ying-Kui Zhao. Movement of ablated high-Z plasmas [J]. Acta Physica Sinica, 2019, 68(18): 185201-1
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